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首页> 外文期刊>Journal of Radioanalytical and Nuclear Chemistry: An International Journal Dealing with All Aspects and Applications of Nuclear Chemistry >Measurements of the thermal neutron cross-sections and resonance integrals for ~(186)W (n,γ) ~(187)W and ~(98)Mo (n,γ) ~(99)Mo reactions
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Measurements of the thermal neutron cross-sections and resonance integrals for ~(186)W (n,γ) ~(187)W and ~(98)Mo (n,γ) ~(99)Mo reactions

机译:〜(186)W(n,γ)〜(187)W和〜(98)Mo(n,γ)〜(99)Mo反应的热中子截面和共振积分的测量

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The thermal neutron cross-sections and resonance integrals of the ~(186)W (n,γ) ~(187)W and ~(98)Mo (n,γ) ~(99)Mo reactions in the thermal and 1/E regions, respectively, of a thermal reactor neutron spectrum have been experimentally determined by the activation method using ~(197)Au (n,γ) ~(198)Au reaction as a single comparator. The high purity natural W, Mo, and Zr foils; and Au wire diluted in aluminum, were irradiated without Cd shield in two neutron irradiation sites, characterized with different values for the thermal-to-epithermal flux ratios, f at the Second Egyptian Research Reactor (ETRR-2). The induced activities in the samples were measured by high-resolution γ-ray spectrometry with a calibrated germanium detector. Thermal neutron cross-sections for 2200 m/s neutrons and resonance integrals for the ~(186)W (n,γ) ~(187)W and ~(98)Mo (n,γ) ~(99)Mo reactions have been obtained relative to the reference values, σ_0 = 98.65 ± 0.09 b and I _0 = 1500 ± 28 b for the ~(197)Au (n,γ) ~(198)Au reaction. The necessary correction factors for thermal neutron and resonance neutron self-shielding effects, and the epithermal flux index (α) were taken into account in the determinations. The results obtained were: σ_0 = 38.43 ± 0.4 b and I _0 = 502 ± 65 b for ~(186)W (n,γ) ~(187)W, and σ_0 = 0.137 ± 0.014 band I _0 = 6.47 ± 0.8 for ~(98)Mo (n,γ) ~(99)Mo. These results are discussed and compared with previous measurements and evaluated data in literature. The traditional method of determining thermal cross-sections and resonance integrals via neutron irradiation with and without Cd shield in one irradiation position was avoided in this work by neutron irradiation without Cd shield in at least two different neutron irradiation positions. This method provides alternative way for determining thermal cross-sections and resonance integrals simultaneously.
机译:〜(186)W(n,γ)〜(187)W和〜(98)Mo(n,γ)〜(99)Mo在热和1 / E反应中的热中子截面和共振积分通过〜(197)Au(n,γ)〜(198)Au反应作为单个比较器的活化方法,分别通过实验确定了热反应堆中子光谱的两个区域。高纯度天然W,Mo和Zr箔;在两个埃及中子辐照位置,在没有Cd防护的情况下辐照铝和稀释在铝中的金丝,其特征在于第二埃及研究堆(ETRR-2)的热-表热通量比f不同。样品中的诱导活性通过使用校准的锗检测器的高分辨率γ射线光谱法进行测量。 2200 m / s中子的热中子截面和〜(186)W(n,γ)〜(187)W和〜(98)Mo(n,γ)〜(99)Mo反应的共振积分已经对于〜(197)Au(n,γ)〜(198)Au反应,相对于参考值σ_0= 98.65±0.09 b和I _0 = 1500±28 b。确定中考虑了热中子和共振中子自屏蔽效应的必要校正因子以及超热通量指数(α)。获得的结果为:对于((186)W(n,γ)〜(187)W),σ_0= 38.43±0.4 b和I _0 = 502±65 b,对于σ_0= 0.137±0.014波段I _0 = 6.47±0.8 〜(98)Mo(n,γ)〜(99)Mo。对这些结果进行了讨论,并与以前的测量结果和文献中的评估数据进行了比较。在这项工作中,通过在至少两个不同的中子辐照位置进行无Cd防护的中子辐照,避免了通过在一个辐照位置进行或不进行Cd防护的中子辐照确定热截面和共振积分的传统方法。该方法为同时确定热截面和共振积分提供了另一种方法。

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